Characterization of the n-TOF EAR-2 neutron beam
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Author
Chen, Y. H.
Tassan-Got, L.
Audouin, L.
Le Naour, C.
Durán, I.
Casarejos, E.
Aberle, O.
Andrzejewski, J.
Bécares, V.
Bacak, M.
Balibrea, J.
Barbagallo, M.
Barros, S.
Bečvář, F.
Beinrucker, C.
Berthoumieux, E.
Billowes, J.
Bosnar, D.
Brugger, M.
Caamaño, M.
Calviño, F.
Calviani, M.
Cano-Ott, D.
Cardella, R.
Casanovas, A.
Castelluccio, D. M.
Cerutti, F.
Chiaveri, E.
Colonna, N.
Cortés, G.
Cortés-Giraldo, M. A.
Cosentino, L.
Damone, L. A.
Diakaki, M.
Domingo-Pardo, C.
Dressler, R.
Dupont, E.
Fernández-Domínguez, B.
Ferrari, A.
Ferreira, P.
Finocchiaro, P.
Furman, V.
Göbel, K.
Gómez-Hornillos, M. B.
García, A. R.
Gawlik, A.
Glodariu, T.
Gonçalves, I. F.
González, E.
Goverdovski, A.
Griesmayer, E.
Guerrero, C.
Gunsing, F.
Harada, H.
Heftrich, T.
Heinitz, S.
Heyse, J.
Jenkins, D. G.
Jericha, E.
Käppeler, F.
Kadi, Y.
Katabuchi, T.
Kavrigin, P.
Ketlerov, V.
Khryachkov, V.
Kimura, A.
Kivel, N.
Kokkoris, M.
Krtička, M.
Leal-Cidoncha, E.
Lederer, C.
Leeb, H.
Lerendegui-Marco, J.
Meo, S. Lo
Lonsdale, S. J.
Losito, R.
Macina, D.
Marganiec, J.
Martínez, T.
Massimi, C.
Mastinu, P.
Mastromarco, M.
Matteucci, F.
Maugeri, E. A.
Mendoza, E.
Mengoni, A.
Milazzo, P. M.
Mingrone, F.
Mirea, M.
Montesano, S.
Musumarra, A.
Nolte, R.
Oprea, A.
Patronis, N.
Pavlik, A.
Perkowski, J.
Porras, J. I.
Praena, J.
Quesada, J. M.
Rajeev, K.
Rauscher, T.
Reifarth, R.
Riego-Perez, A.
Robles, M.
Rout, P. C.
Rubbia, C.
Ryan, J. A.
Sabaté-Gilarte, M.
Saxena, A.
Schillebeeckx, P.
Schmidt, S.
Schumann, D.
Sedyshev, P.
Smith, A. G.
Stamatopoulos, A.
Tagliente, G.
Tain, J. L.
Tarifeño-Saldivia, A.
Tsinganis, A.
Valenta, S.
Vannini, G.
Variale, V.
Vaz, P.
Ventura, A.
Vlachoudis, V.
Vlastou, R.
Wallner, A.
Warren, S.
Weigand, M.
Weiss, C.
Wolf, C.
Woods, P. J.
Wright, T.
Ugec, P.
Attention
2299/21761
Abstract
The experimental area 2 (EAR-2) at CERNs neutron time-of-flight facility (n-TOF), which is operational since 2014, is designed and built as a short-distance complement to the experimental area 1 (EAR-1). The Parallel Plate Avalanche Counter (PPAC) monitor experiment was performed to characterize the beam prole and the shape of the neutron 'ux at EAR-2. The prompt γ-flash which is used for calibrating the time-of-flight at EAR-1 is not seen by PPAC at EAR-2, shedding light on the physical origin of this γ-flash.